We examine the shift in the chiral condensate due to a constant electromagnetic field at O(p(6)) using SU(2) chiral perturbation theory and a realistic M-pi=140 MeV. We find that this value differs significantly from the value calculated using M-pi=0, while the magnitude of the two-loop correction is unclear due to the uncertainty in the experimentally determined value of the relevant L-6 LEC.
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